Josephson Junctions: Is There a Contradiction?

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In summary, the resistance is zero at zero bias in the I-V curve, but the conductance is finite due to Andreev reflection. This is a quantum phenomenon explained by the macroscopic wave function and the Josephson relation for current density. Andreev reflection is not observed at zero bias, only in highly transparent junctions.
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Recently I am confused about this thing: according to the I-V curve, the resistance is 0 at zero bias, however, the conductance is finite by Andreev reflection? Is there a contradictory? Thanks!
 
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Hi,

You should think this phenomena not in the classical picture but as a quantum phenomena where this effect is due to a Macroscopic Wave Function, just as an example you can think as an electron "turns" around the nuclei, it does not loss any energy.
Finally remember that in the Josephson equations the current is more an oscillation where current goes back and forth keeping the mean current equal to zero.
Cheers
 
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JJ zero bias conductance

The current through the JJ is due to tunneling of Cooper pairs. Unlike quasiparticle tunneling, pair tunneling does not involve excitations and can occur even without bias across the junction. Thus one
could connect a current source to a junction and, for currents less than a certain critical value, no
voltage would be developed if the current were carried across the insulator by Cooper pairs. The tunnel current is mediated by the phase difference of the macroscopic wave function across the junction and expressed in the Josephson relation for the current density: J = (Jc)sin(phi), where Jc is the critical current density and phi is the phase difference.

Andreev reflection is only observed in junctions with an highly transparent tunnel barrier (oxide barriers disrupt the coherent quasiparticle scattering channel) and is not observed at zero bias.
 

1. What are Josephson junctions and how do they work?

Josephson junctions are a type of superconducting device that consists of two superconducting materials separated by a thin insulating barrier. They work by allowing the flow of supercurrent, a phenomenon where electrons pair up and move through the junction without resistance.

2. What is the contradiction surrounding Josephson junctions?

The contradiction surrounding Josephson junctions is that they exhibit both classical and quantum mechanical behaviors, which seems to contradict the laws of physics.

3. How can Josephson junctions exhibit both classical and quantum behaviors?

This contradiction is resolved by the theory of macroscopic quantum coherence, which explains that the behavior of a large number of quantum particles can appear classical. In Josephson junctions, the supercurrent involves a large number of paired electrons, making it a macroscopic phenomenon.

4. What are the practical applications of Josephson junctions?

Josephson junctions have various applications in electronics, particularly in the development of high-speed and low-noise devices. They are also used in quantum computing, as their ability to exhibit both classical and quantum behaviors make them ideal for processing and storing quantum information.

5. Are there any limitations or challenges in using Josephson junctions?

While Josephson junctions have many potential applications, they also face challenges such as maintaining their superconducting state in high temperatures and avoiding interference from external magnetic fields. Additionally, the fabrication process for these devices can be complex and costly.

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